<p>We study the boundedness of wave operators associated with one-dimensional Schrödinger operators with a generalized point interaction. Let <i>H</i> denote the Laplacian with a generalized point interaction at the origin and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(H_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> the free Hamiltonian in <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(L^2({\mathbb {R}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. In this paper, we prove that the wave operators <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(W_\pm (H,H_0)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>W</mi> <mo>±</mo> </msub> <mrow> <mo stretchy="false">(</mo> <mi>H</mi> <mo>,</mo> <msub> <mi>H</mi> <mn>0</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> are extended to bounded operators on the Sobolev spaces <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(W^{k,p}(\mathbb {R})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>W</mi> <mrow> <mi>k</mi> <mo>,</mo> <mi>p</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(k=0,1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>k</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(1&lt;p&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. The boundedness of wave operators has been established for Schrödinger operators with decaying potentials by Yajima [<CitationRef CitationID="CR25">25</CitationRef>, <CitationRef CitationID="CR26">26</CitationRef>] and Weder [<CitationRef CitationID="CR24">24</CitationRef>] and for certain singular perturbations such as <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\delta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>δ</mi> </math></EquationSource> </InlineEquation>-interactions by Duchêne et al. [<CitationRef CitationID="CR9">9</CitationRef>]. The present result shows that the boundedness extends to the whole class of generalized point interactions.</p>

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The \(W^{1,p}\)-continuity of the wave operators for the one-dimensional Schrödinger operators with a generalized point interaction

  • Hiroaki Niikuni

摘要

We study the boundedness of wave operators associated with one-dimensional Schrödinger operators with a generalized point interaction. Let H denote the Laplacian with a generalized point interaction at the origin and \(H_0\) H 0 the free Hamiltonian in \(L^2({\mathbb {R}})\) L 2 ( R ) . In this paper, we prove that the wave operators \(W_\pm (H,H_0)\) W ± ( H , H 0 ) are extended to bounded operators on the Sobolev spaces \(W^{k,p}(\mathbb {R})\) W k , p ( R ) for \(k=0,1\) k = 0 , 1 and \(1<p<\infty \) 1 < p < . The boundedness of wave operators has been established for Schrödinger operators with decaying potentials by Yajima [25, 26] and Weder [24] and for certain singular perturbations such as \(\delta \) δ -interactions by Duchêne et al. [9]. The present result shows that the boundedness extends to the whole class of generalized point interactions.